Notes on Principal Bundles and Classifying Spaces

Total Page:16

File Type:pdf, Size:1020Kb

Notes on Principal Bundles and Classifying Spaces Notes on principal bundles and classifying spaces Stephen A. Mitchell June 2011 1 Introduction Consider a real n-plane bundle ξ with Euclidean metric. Associated to ξ are a number of auxiliary bundles: disc bundle, sphere bundle, projective bundle, k-frame bundle, etc. Here \bundle" simply means a local product with the indicated fibre. In each case one can show, by easy but repetitive arguments, that the projection map in question is indeed a local product; furthermore, the transition functions are always linear in the sense that they are induced in an obvious way from the linear transition functions of ξ. It turns out that all of this data can be subsumed in a single object: the \principal O(n)-bundle" Pξ, which is just the bundle of orthonormal n-frames. The fact that the transition functions of the various associated bundles are linear can then be formalized in the notion “fibre bundle with structure group O(n)". If we do not want to consider a Euclidean metric, there is an analogous notion of principal GLnR-bundle; this is the bundle of linearly independent n-frames. More generally, if G is any topological group, a principal G-bundle is a locally trivial free G-space with orbit space B (see below for the precise definition). For example, if G is discrete then a principal G-bundle with connected total space is the same thing as a regular covering map with G as group of deck transformations. Under mild hypotheses there exists a classifying space BG, such that isomorphism classes of principal G-bundles over X are in natural bijective correspondence with [X; BG]. The correspondence is given by pulling back a universal principal G-bundle over BG. When G is discrete, BG is an Eilenberg-Maclane space of type (G; 1). When G is either GLnR or O(n), BG is homotopy equivalent to the 1 infinite Grassmanian GnR . The homotopy classification theorem for vector bundles then emerges as a special case of the homotopy classification theorem for principal bundles. As these examples begin to suggest, the concept principal bundle acts as a powerful unifying force in algebraic topology. Classifying spaces also play a central role; indeed, much of the research in homotopy theory over the last fifty years involves analyzing the homotopy- type of BG for interesting groups G. There are also many applications in differential geometry, involving connections, curvature, etc. In these notes we will study principal bundles and classifying spaces from the homotopy-theoretic point of view. 1 2 Definitions and basic properties Let G be a topological group. A left G-space is a space X equipped with a continuous left G-action G×X −! X. If X and Y are G-spaces, a G-equivariant map is a map φ : X −! Y such that φ(gx) = gφ(x) for all g 2 G; x 2 X. Synonymous terms include equivariant (if the group G is understood) and G-map (for short). This makes left G-spaces into a category. A G-homotopy (or G-equivariant homotopy, or equivariant homotopy) between G-maps φ, is a homotopy F : X × I −! Y in the usual sense, with the added condition that F be G- equivariant (here G acts trivially on the I coordinate). This yields the G-homotopy category of left G-spaces. Similar definitions apply to right G-spaces. Now let B be a topological space. Suppose that P is a right G-space equipped with a G-map π : P −! B, where G acts trivially on B (in other words, π factors uniquely through the orbit space P=G). We say that (P; π) is a principal G-bundle over B if π satisfies the following local triviality condition: B has a covering by open sets U such that there exist G-equivariant homeomorphisms −1 φU : π U −! U × G commuting in the diagram φ π−1U U- U × G ? © U Here U × G has the right G-action (u; g)h = (u; gh). Note this condition implies that G acts freely on P, and that π factors through a homeomorphism π : P=G −! B (thus B \is" the orbit space of P). Summarizing: A principal G-bundle over B consists of a locally trivial free G-space with orbit space B. A morphism of principal bundles over B is an equivariant map σ : P −! Q over the identity of B (i.e., inducing the identity map on the orbit space). This makes the collection of all principal G-bundles over B into a category. The set of isomorphism classes of principal G-bundles over B will be denote PGB. A principal G-bundle is trivial if it is isomorphic to the product principal bundle B × G −! B. Every principal bundle is locally trivial, by definition. Note that (P; π) is in particular a local product over B with fibre G. To be a principal G- bundle, however, is a far stronger condition. Here are two striking and important properties that illustrate this claim: Proposition 2.1 Any morphism of principal G-bundles is an isomorphism. Proof: Let σ : P −! Q be a morphism. Suppose first that P = Q = B × G. Then σ(b; g) = (b; f(b)g) for some function f : B −! G; clearly f is continuous. Hence σ is an isomorphism with σ−1(b; g) = (b; f(b)−1g). This proves the proposition in the case when P and Q are trivial. Since every principal bundle is locally trivial, the general case follows immediately. 2 Proposition 2.2 A principal G-bundle π : P −! B is trivial if and only if it admits a section. Proof: If P is trivial, then there is a section; this much is trivially true for any local product. Conversely, suppose s : B −! P is a section. Then the map φ : B × G −! P given by φ(b; g) = s(b)g is a morphism of principal bundles, and is therefore an isomorphism by Proposition 2.1. The difference between a principal G-bundle and a run-of-the-mill local product with fibre G can be illustrated further in terms of transition functions. Suppose π : E −! B is a local product with fibre G, and U,V are open sets over which π is trivial, with U \ V nonempty. Comparing the two trivializations leads to a homeomorphism (U \ V ) × G −! (U \ V ) × G of the form (x; g) 7! (x; φ(x)g), where the transition function φ is a map from U \V into the set of homeomorphisms from G to itself. In a principal G-bundle, each φ(x) is left translation by an element of G, and φ : U \ V −! G is continuous. Given a principal G-bundle P over B and a map f : B0 −! B, we can form the pullback 0 ∗ 0 P ≡ f P ≡ B ×B P ; the pullback inherits a natural structure of principal G-bundle over B0 from P. The reader should note the following two simple and purely categorical facts: First, if Q is a principal G-bundle over B0, then bundle maps Q −! f ∗P are in bijective correspondence with commutative squares Q - P ? ? B0 - B in which the top arrow is a G-equivariant map. Second, sections of the pullback bundle f ∗P are in bijective correspondence with lifts in the diagram P p p p ? p p 0 p p - B B p f We conclude this section with an interesting special case of the pullback construction. We can pull P back over itself: π00- P ×B P P π0 π ? ? - PBπ Here π0 is projection on the lefthand factor, and defines a principal G-bundle structure in which the G-action on P ×B P is on the righthand factor. 3 0 Proposition 2.3 π : P ×B P −! P is a trivial principal G-bundle over P. Proof: The diagonal map P −! P ×B P is a section; now apply Proposition 2.2. Note that the trivialization obtained is the map P × G −! P ×B P given by (p; g) 7! (p; pg). By symmetry, a similar result holds for π00, with the roles of the left and right factors reversed. 3 Balanced products and fiber bundles with structure group Note that any left G-action on a space X can be converted to right action|and vice-versa| by setting xg = g−1x, x 2 X. If W is a right G-space and X is a left G-space, the balanced product W ×GX is the quotient space W × X= ∼, where (wg; x) ∼ (w; gx). Equivalently, we can simply convert X to a right G-space as above, and take the orbit space of the diagonal action (w; x)g = (wg; g−1x); thus W ×G X = (W × X)=G. The following special cases should be noted: (i) If X = ∗ is a point, W ×G ∗ = W=G. (ii) If X = G with the left translation action, the right action of G on itself makes W ×G G into a right G-space, and the action map W × G −! W induces a G-equivariant =∼ homeomorphism W ×G G −! W . Let G,H be topological groups. A (G,H)-space is a space Y equipped with a left G-action and right H-action, such that the two actions commute: (gy)h = g(yh). If we convert (say) the right H-action to a left action, this is the same thing as a left G × H-action. Note that if Y is a (G,H)-space and X is a right G-space, X ×G Y receives a right H-action defined by [x; y]h = [x; yh]; similarly Y ×H Z has a left G-action if Z is a left H-space.
Recommended publications
  • Orientability of Real Parts and Spin Structures
    JP Jour. Geometry & Topology 7 (2007) 159-174 ORIENTABILITY OF REAL PARTS AND SPIN STRUCTURES SHUGUANG WANG Abstract. We establish the orientability and orientations of vector bundles that arise as the real parts of real structures by utilizing spin structures. 1. Introduction. Unlike complex algebraic varieties, real algebraic varieties are in general nonorientable, the simplest example being the real projective plane RP2. Even if they are orientable, there may not be canonical orientations. It has been an important problem to resolve the orientability and orientation issues in real algebraic geometry. In 1974, Rokhlin introduced the complex orientation for dividing real algebraic curves in RP2, which was then extended around 1982 by Viro to the so-called type-I real algebraic surfaces. A detailed historic count was presented in the lucid survey by Viro [10], where he also made some speculations on higher dimensional varieties. In this short note, we investigate the following more general situation. We take σ : X → X to be a smooth involution on a smooth manifold of an arbitrary dimension. (It is possible to consider involutions on topological manifolds with appropriate modifications.) Henceforth, we will assume that X is connected for certainty. In view of the motivation above, let us denote the fixed point set by XR, which in general is disconnected and will be assumed to be non-empty throughout the paper. Suppose E → X is a complex vector bundle and assume σ has an involutional lifting σE on E that is conjugate linear fiberwise. We call σE a real structure on E and its fixed point set ER a real part.
    [Show full text]
  • The Stable Homotopy of Complex Projective Space
    THE STABLE HOMOTOPY OF COMPLEX PROJECTIVE SPACE By GRAEME SEGAL [Received 17 March 1972] 1. Introduction THE object of this note is to prove that the space BU is a direct factor of the space Q(CP°°) = Oto5eo(CP00) = HmQn/Sn(CPto). This is not very n surprising, as Toda [cf. (6) (2.1)] has shown that the homotopy groups of ^(CP00), i.e. the stable homotopy groups of CP00, split in the appro- priate way. But the method, which is Quillen's technique (7) of reducing to a problem about finite groups and then using the Brauer induction theorem, may be interesting. If X and Y are spaces, I shall write {X;7}*for where Y+ means Y together with a disjoint base-point, and [ ; ] means homotopy classes of maps with no conditions about base-points. For fixed Y, X i-> {X; Y}* is a representable cohomology theory. If Y is a topological abelian group the composition YxY ->Y induces and makes { ; Y}* into a multiplicative cohomology theory. In fact it is easy to see that {X; Y}° is then even a A-ring. Let P = CP00, and embed it in the space ZxBU which represents the functor K by P — IXBQCZXBU. This corresponds to the natural inclusion {line bundles} c {virtual vector bundles}. There is an induced map from the suspension-spectrum of P to the spectrum representing l£-theory, inducing a transformation of multiplicative cohomology theories T: { ; P}* -*• K*. PROPOSITION 1. For any space, X the ring-homomorphism T:{X;P}°-*K<>(X) is mirjective. COEOLLAKY. The space QP is (up to homotopy) the product of BU and a space with finite homotopy groups.
    [Show full text]
  • Horizontal Holonomy and Foliated Manifolds Yacine Chitour, Erlend Grong, Frédéric Jean, Petri Kokkonen
    Horizontal holonomy and foliated manifolds Yacine Chitour, Erlend Grong, Frédéric Jean, Petri Kokkonen To cite this version: Yacine Chitour, Erlend Grong, Frédéric Jean, Petri Kokkonen. Horizontal holonomy and foliated manifolds. Annales de l’Institut Fourier, Association des Annales de l’Institut Fourier, 2019, 69 (3), pp.1047-1086. 10.5802/aif.3265. hal-01268119 HAL Id: hal-01268119 https://hal-ensta-paris.archives-ouvertes.fr//hal-01268119 Submitted on 8 Mar 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. HORIZONTAL HOLONOMY AND FOLIATED MANIFOLDS YACINE CHITOUR, ERLEND GRONG, FRED´ ERIC´ JEAN AND PETRI KOKKONEN Abstract. We introduce horizontal holonomy groups, which are groups de- fined using parallel transport only along curves tangent to a given subbundle D of the tangent bundle. We provide explicit means of computing these holo- nomy groups by deriving analogues of Ambrose-Singer's and Ozeki's theorems. We then give necessary and sufficient conditions in terms of the horizontal ho- lonomy groups for existence of solutions of two problems on foliated manifolds: determining when a foliation can be either (a) totally geodesic or (b) endowed with a principal bundle structure.
    [Show full text]
  • Stable Higgs Bundles on Ruled Surfaces 3
    STABLE HIGGS BUNDLES ON RULED SURFACES SNEHAJIT MISRA Abstract. Let π : X = PC(E) −→ C be a ruled surface over an algebraically closed field k of characteristic 0, with a fixed polarization L on X. In this paper, we show that pullback of a (semi)stable Higgs bundle on C under π is a L-(semi)stable Higgs bundle. Conversely, if (V,θ) ∗ is a L-(semi)stable Higgs bundle on X with c1(V ) = π (d) for some divisor d of degree d on C and c2(V ) = 0, then there exists a (semi)stable Higgs bundle (W, ψ) of degree d on C whose pullback under π is isomorphic to (V,θ). As a consequence, we get an isomorphism between the corresponding moduli spaces of (semi)stable Higgs bundles. We also show the existence of non-trivial stable Higgs bundle on X whenever g(C) ≥ 2 and the base field is C. 1. Introduction A Higgs bundle on an algebraic variety X is a pair (V, θ) consisting of a vector bundle V 1 over X together with a Higgs field θ : V −→ V ⊗ ΩX such that θ ∧ θ = 0. Higgs bundle comes with a natural stability condition (see Definition 2.3 for stability), which allows one to study the moduli spaces of stable Higgs bundles on X. Higgs bundles on Riemann surfaces were first introduced by Nigel Hitchin in 1987 and subsequently, Simpson extended this notion on higher dimensional varieties. Since then, these objects have been studied by many authors, but very little is known about stability of Higgs bundles on ruled surfaces.
    [Show full text]
  • LECTURE 6: FIBER BUNDLES in This Section We Will Introduce The
    LECTURE 6: FIBER BUNDLES In this section we will introduce the interesting class of fibrations given by fiber bundles. Fiber bundles play an important role in many geometric contexts. For example, the Grassmaniann varieties and certain fiber bundles associated to Stiefel varieties are central in the classification of vector bundles over (nice) spaces. The fact that fiber bundles are examples of Serre fibrations follows from Theorem ?? which states that being a Serre fibration is a local property. 1. Fiber bundles and principal bundles Definition 6.1. A fiber bundle with fiber F is a map p: E ! X with the following property: every ∼ −1 point x 2 X has a neighborhood U ⊆ X for which there is a homeomorphism φU : U × F = p (U) such that the following diagram commutes in which π1 : U × F ! U is the projection on the first factor: φ U × F U / p−1(U) ∼= π1 p * U t Remark 6.2. The projection X × F ! X is an example of a fiber bundle: it is called the trivial bundle over X with fiber F . By definition, a fiber bundle is a map which is `locally' homeomorphic to a trivial bundle. The homeomorphism φU in the definition is a local trivialization of the bundle, or a trivialization over U. Let us begin with an interesting subclass. A fiber bundle whose fiber F is a discrete space is (by definition) a covering projection (with fiber F ). For example, the exponential map R ! S1 is a covering projection with fiber Z. Suppose X is a space which is path-connected and locally simply connected (in fact, the weaker condition of being semi-locally simply connected would be enough for the following construction).
    [Show full text]
  • FOLIATIONS Introduction. the Study of Foliations on Manifolds Has a Long
    BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 80, Number 3, May 1974 FOLIATIONS BY H. BLAINE LAWSON, JR.1 TABLE OF CONTENTS 1. Definitions and general examples. 2. Foliations of dimension-one. 3. Higher dimensional foliations; integrability criteria. 4. Foliations of codimension-one; existence theorems. 5. Notions of equivalence; foliated cobordism groups. 6. The general theory; classifying spaces and characteristic classes for foliations. 7. Results on open manifolds; the classification theory of Gromov-Haefliger-Phillips. 8. Results on closed manifolds; questions of compact leaves and stability. Introduction. The study of foliations on manifolds has a long history in mathematics, even though it did not emerge as a distinct field until the appearance in the 1940's of the work of Ehresmann and Reeb. Since that time, the subject has enjoyed a rapid development, and, at the moment, it is the focus of a great deal of research activity. The purpose of this article is to provide an introduction to the subject and present a picture of the field as it is currently evolving. The treatment will by no means be exhaustive. My original objective was merely to summarize some recent developments in the specialized study of codimension-one foliations on compact manifolds. However, somewhere in the writing I succumbed to the temptation to continue on to interesting, related topics. The end product is essentially a general survey of new results in the field with, of course, the customary bias for areas of personal interest to the author. Since such articles are not written for the specialist, I have spent some time in introducing and motivating the subject.
    [Show full text]
  • Math 704: Part 1: Principal Bundles and Connections
    MATH 704: PART 1: PRINCIPAL BUNDLES AND CONNECTIONS WEIMIN CHEN Contents 1. Lie Groups 1 2. Principal Bundles 3 3. Connections and curvature 6 4. Covariant derivatives 12 References 13 1. Lie Groups A Lie group G is a smooth manifold such that the multiplication map G × G ! G, (g; h) 7! gh, and the inverse map G ! G, g 7! g−1, are smooth maps. A Lie subgroup H of G is a subgroup of G which is at the same time an embedded submanifold. A Lie group homomorphism is a group homomorphism which is a smooth map between the Lie groups. The Lie algebra, denoted by Lie(G), of a Lie group G consists of the set of left-invariant vector fields on G, i.e., Lie(G) = fX 2 X (G)j(Lg)∗X = Xg, where Lg : G ! G is the left translation Lg(h) = gh. As a vector space, Lie(G) is naturally identified with the tangent space TeG via X 7! X(e). A Lie group homomorphism naturally induces a Lie algebra homomorphism between the associated Lie algebras. Finally, the universal cover of a connected Lie group is naturally a Lie group, which is in one to one correspondence with the corresponding Lie algebras. Example 1.1. Here are some important Lie groups in geometry and topology. • GL(n; R), GL(n; C), where GL(n; C) can be naturally identified as a Lie sub- group of GL(2n; R). • SL(n; R), O(n), SO(n) = O(n) \ SL(n; R), Lie subgroups of GL(n; R).
    [Show full text]
  • Notes on Principal Bundles and Classifying Spaces
    Notes on principal bundles and classifying spaces Stephen A. Mitchell August 2001 1 Introduction Consider a real n-plane bundle ξ with Euclidean metric. Associated to ξ are a number of auxiliary bundles: disc bundle, sphere bundle, projective bundle, k-frame bundle, etc. Here “bundle” simply means a local product with the indicated fibre. In each case one can show, by easy but repetitive arguments, that the projection map in question is indeed a local product; furthermore, the transition functions are always linear in the sense that they are induced in an obvious way from the linear transition functions of ξ. It turns out that all of this data can be subsumed in a single object: the “principal O(n)-bundle” Pξ, which is just the bundle of orthonormal n-frames. The fact that the transition functions of the various associated bundles are linear can then be formalized in the notion “fibre bundle with structure group O(n)”. If we do not want to consider a Euclidean metric, there is an analogous notion of principal GLnR-bundle; this is the bundle of linearly independent n-frames. More generally, if G is any topological group, a principal G-bundle is a locally trivial free G-space with orbit space B (see below for the precise definition). For example, if G is discrete then a principal G-bundle with connected total space is the same thing as a regular covering map with G as group of deck transformations. Under mild hypotheses there exists a classifying space BG, such that isomorphism classes of principal G-bundles over X are in natural bijective correspondence with [X, BG].
    [Show full text]
  • Group Invariant Solutions Without Transversality 2 in Detail, a General Method for Characterizing the Group Invariant Sections of a Given Bundle
    GROUP INVARIANT SOLUTIONS WITHOUT TRANSVERSALITY Ian M. Anderson Mark E. Fels Charles G. Torre Department of Mathematics Department of Mathematics Department of Physics Utah State University Utah State University Utah State University Logan, Utah 84322 Logan, Utah 84322 Logan, Utah 84322 Abstract. We present a generalization of Lie’s method for finding the group invariant solutions to a system of partial differential equations. Our generalization relaxes the standard transversality assumption and encompasses the common situation where the reduced differential equations for the group invariant solutions involve both fewer dependent and independent variables. The theoretical basis for our method is provided by a general existence theorem for the invariant sections, both local and global, of a bundle on which a finite dimensional Lie group acts. A simple and natural extension of our characterization of invariant sections leads to an intrinsic characterization of the reduced equations for the group invariant solutions for a system of differential equations. The char- acterization of both the invariant sections and the reduced equations are summarized schematically by the kinematic and dynamic reduction diagrams and are illustrated by a number of examples from fluid mechanics, harmonic maps, and general relativity. This work also provides the theoretical foundations for a further detailed study of the reduced equations for group invariant solutions. Keywords. Lie symmetry reduction, group invariant solutions, kinematic reduction diagram, dy- namic reduction diagram. arXiv:math-ph/9910015v2 13 Apr 2000 February , Research supported by NSF grants DMS–9403788 and PHY–9732636 1. Introduction. Lie’s method of symmetry reduction for finding the group invariant solutions to partial differential equations is widely recognized as one of the most general and effective methods for obtaining exact solutions of non-linear partial differential equations.
    [Show full text]
  • Composable Geometric Motion Policies Using Multi-Task Pullback Bundle Dynamical Systems
    Composable Geometric Motion Policies using Multi-Task Pullback Bundle Dynamical Systems Andrew Bylard, Riccardo Bonalli, Marco Pavone Abstract— Despite decades of work in fast reactive plan- ning and control, challenges remain in developing reactive motion policies on non-Euclidean manifolds and enforcing constraints while avoiding undesirable potential function local minima. This work presents a principled method for designing and fusing desired robot task behaviors into a stable robot motion policy, leveraging the geometric structure of non- Euclidean manifolds, which are prevalent in robot configuration and task spaces. Our Pullback Bundle Dynamical Systems (PBDS) framework drives desired task behaviors and prioritizes tasks using separate position-dependent and position/velocity- dependent Riemannian metrics, respectively, thus simplifying individual task design and modular composition of tasks. For enforcing constraints, we provide a class of metric-based tasks, eliminating local minima by imposing non-conflicting potential functions only for goal region attraction. We also provide a geometric optimization problem for combining tasks inspired by Riemannian Motion Policies (RMPs) that reduces to a simple least-squares problem, and we show that our approach is geometrically well-defined. We demonstrate the 2 PBDS framework on the sphere S and at 300-500 Hz on a manipulator arm, and we provide task design guidance and an open-source Julia library implementation. Overall, this work Fig. 1: Example tree of PBDS task mappings designed to move a ball along presents a fast, easy-to-use framework for generating motion the surface of a sphere to a goal while avoiding obstacles. Depicted are policies without unwanted potential function local minima on manifolds representing: (black) joint configuration for a 7-DoF robot arm general manifolds.
    [Show full text]
  • Lectures on the Stable Homotopy of BG 1 Preliminaries
    Geometry & Topology Monographs 11 (2007) 289–308 289 arXiv version: fonts, pagination and layout may vary from GTM published version Lectures on the stable homotopy of BG STEWART PRIDDY This paper is a survey of the stable homotopy theory of BG for G a finite group. It is based on a series of lectures given at the Summer School associated with the Topology Conference at the Vietnam National University, Hanoi, August 2004. 55P42; 55R35, 20C20 Let G be a finite group. Our goal is to study the stable homotopy of the classifying space BG completed at some prime p. For ease of notation, we shall always assume that any space in question has been p–completed. Our fundamental approach is to decompose the stable type of BG into its various summands. This is useful in addressing many questions in homotopy theory especially when the summands can be identified with simpler or at least better known spaces or spectra. It turns out that the summands of BG appear at various levels related to the subgroup lattice of G. Moreover since we are working at a prime, the modular representation theory of automorphism groups of p–subgroups of G plays a key role. These automorphisms arise from the normalizers of these subgroups exactly as they do in p–local group theory. The end result is that a complete stable decomposition of BG into indecomposable summands can be described (Theorem 6) and its stable homotopy type can be characterized algebraically (Theorem 7) in terms of simple modules of automorphism groups. This paper is a slightly expanded version of lectures given at the International School of the Hanoi Conference on Algebraic Topology, August 2004.
    [Show full text]
  • The Classifying Space of the G-Cobordism Category in Dimension Two
    The classifying space of the G-cobordism category in dimension two Carlos Segovia Gonz´alez Instituto de Matem´aticasUNAM Oaxaca, M´exico 29 January 2019 The classifying space I Graeme Segal, Classifying spaces and spectral sequences (1968) I A. Grothendieck, Th´eorie de la descente, etc., S´eminaire Bourbaki,195 (1959-1960) I S. Eilenberg and S. MacLane, Relations between homology and homotopy groups of spaces I and II (1945-1950) I P.S. Aleksandrov-E.Chec,ˇ Nerve of a covering (1920s) I B. Riemann, Moduli space (1857) Definition A simplicial set X is a contravariant functor X : ∆ ! Set from the simplicial category to the category of sets. The geometric realization, denoted by jX j, is the topological space defined as ` jX j := n≥0(∆n × Xn)= ∼, where (s; X (f )a) ∼ (∆f (s); a) for all s 2 ∆n, a 2 Xm, and f :[n] ! [m] in ∆. Definition For a small category C we define the simplicial set N(C), called the nerve, denoted by N(C)n := Fun([n]; C), which consists of all the functors from the category [n] to C. The classifying space of C is the geometric realization of N(C). Denote this by BC := jN(C)j. Properties I The functor B : Cat ! Top sends a category to a topological space, a functor to a continuous map and a natural transformation to a homotopy. 0 0 I B conmutes with products B(C × C ) =∼ BC × BC . I A equivalence of categories gives a homotopy equivalence. I A category with initial or final object is contractil.
    [Show full text]